Imaging lens and imaging apparatus including the imaging lens

ABSTRACT

An imaging lens substantially consists of, in order from an object side, five lenses of a first lens that has a positive refractive power and has a meniscus shape which is convex toward the object side, a second lens that has a negative refractive power, a third lens that has a negative refractive power, a fourth lens that has a positive refractive power, and a fifth lens that has a negative refractive power and has an aspheric shape of which an image side surface has an extreme point. Further, the imaging lens satisfies a predetermined conditional expression.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to a fixed-focus imaging lens that forms an optical image of a subject on an imaging device, such as a charge coupled device (CCD) and a complementary metal oxide semiconductor (CMOS), and to an imaging apparatus, such as a digital still camera, a cellular phone with a camera, a mobile information terminal (PDA: Personal Digital Assistance), a smartphone, a tablet terminal, and a mobile game machine, on which the imaging lens is mounted to perform photography.

2. Description of the Related Art

As personal computers have become popular in homes, digital still cameras which are capable of inputting image information about photographed scenes, persons, and the like into the personal computers have spread rapidly. Further, a cellular phone, a smartphone, or a tablet terminal in which a camera module for inputting images is installed has been increasing. Such apparatus having an imaging function uses an imaging device, such as a CCD and a CMOS. Recently, because the imaging device has been miniaturized, there has been also a demand to miniaturize the whole of the imaging apparatus and an imaging lens mounted thereon. Further, since the number of pixels included in the imaging device has also been increasing, there has been a demand to enhance the resolution and performance of the imaging lens. For example, there has been a demand for performance corresponding to high resolution of 5 megapixels or higher, and preferably performance corresponding to high resolution of 8 megapixels or higher.

To satisfy such demands, it can be considered that the imaging lens is composed of five or six lenses, which are a relatively large number of lenses. For example, U.S. Patent Application Publication No. 20130021680 (Patent Document 1) and U.S. Patent Application Publication No. 20130057968 (Patent Document 2) propose an imaging lens composed of five lenses. The imaging lens disclosed in Patent Documents 1 and 2 substantially consists of, in order from an object side, five lenses of a first lens that has a positive refractive power, a second lens that has a negative refractive power, a third lens that has a negative refractive power, a fourth lens that has a positive refractive power, and a fifth lens that has a negative refractive power.

SUMMARY OF THE INVENTION

In particular, for the imaging lenses used in apparatuses, of which the thickness has been decreased, such as a cellular phone, a smartphone or a tablet terminal, a demand to decrease the total length of the lens has been increased more and more. Hence, it is necessary to further decrease the total lengths of the imaging lenses disclosed in Patent Documents 1 and 2.

The present invention has been made in view of the above-mentioned circumstances and an object thereof is to provide an imaging lens capable of achieving high imaging performance in the range from the central angle of view to the peripheral angle of view while achieving a decrease in the total length thereof. Another object of the present invention is to provide an imaging apparatus capable of obtaining a photographed image with high resolution through the imaging lens which is mounted thereon.

The imaging lens of the present invention is an imaging lens substantially consisting of, in order from an object side, five lenses of:

a first lens that has a positive refractive power and has a meniscus shape which is convex toward the object side;

a second lens that has a negative refractive power;

a third lens that has a negative refractive power;

a fourth lens that has a positive refractive power; and

a fifth lens that has a negative refractive power and has an aspheric shape of which an image side surface has an extreme point,

in which the following conditional expression (1) is satisfied:

−1<f/f45<−0.105  (1), where

f is a focal length of a whole system, and

f45 is a composite focal length of the fourth and fifth lenses.

According to the imaging lens of the present invention, in the imaging lens which is composed of five lenses as a whole, a configuration of each lens element of the first to fifth lenses is optimized. Therefore, it is possible to achieve a lens system that has high resolution performance while decreasing the total length thereof.

In the imaging lens of the present invention, the expression “substantially consisting of five lenses” means that the imaging lens of the present invention may include not only the five lenses but also a lens which has substantially no refractive power, optical elements, such as a stop and a cover glass, which are not a lens, mechanism parts, such as a lens flange, a lens barrel, an imaging device and a hand shake blur correction mechanism, and the like. When the lens includes an aspheric surface, the reference sign of the surface shape and refractive power of the lens is considered in a paraxial region.

In the imaging lens of the present invention, by employing and satisfying the following desirable configuration, it is possible to make the optical performance thereof better.

In the imaging lens of the present invention, it is desirable that among absolute values of respective focal lengths of the first to fifth lenses, an absolute value of a focal length of the third lens be the maximum.

In the imaging lens of the present invention, it is desirable that an intersection point between an object side surface of the forth lens and a principal ray with a maximum angle of view be positioned on the object side of an intersection point between the object side surface of the forth lens and an optical axis.

In the imaging lens of the present invention, it is desirable that an intersection point between an object side surface of the third lens and a principal ray with a maximum angle of view be positioned on the object side of an intersection point between the object side surface of the third lens and the optical axis.

In the imaging lens of the present invention, it is desirable that the second lens be concave toward the image side.

It is desirable that the imaging lens of the present invention satisfy any of the following conditional expressions (1-1) to (2-2). It should be noted that, as a desirable mode, any one of the conditional expressions (1-1) to (2-2) may be satisfied, or an arbitrary combination thereof may be satisfied.

−0.9<f/f45<−0.105  (1-1),

−0.8<f/f45<−0.1  (1-2),

0.02<D6/f<0.3  (2),

0.03<D6/f<0.2  (2-1), and

0.04<D6/f<0.18  (2-2), where

f is a focal length of a whole system,

f45 is a composite focal length of the fourth and fifth lenses, and

D6 is a thickness of the third lens on an optical axis.

The imaging apparatus of the present invention includes the imaging lens of the present invention.

According to the imaging lens of the present invention, in the imaging lens which is composed of five lenses as a whole, a configuration of each lens element is optimized, and particularly the shape of the fifth lens is appropriately formed. Therefore, it is possible to achieve a lens system that has high resolution performance in the range from the central angle of view to the peripheral angle of view while decreasing the total length thereof.

Further, according to the imaging apparatus of the present invention, imaging signals based on an optical image formed by the imaging lens of the present invention, which has high imaging performance, are output. Therefore, it is possible to obtain a photographed image with high resolution.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a lens cross-sectional view illustrating a first configuration example of an imaging lens according to an embodiment of the present invention and corresponding to Example 1;

FIG. 2 is a lens cross-sectional view illustrating a second configuration example of an imaging lens according to an embodiment of the present invention and corresponding to Example 2;

FIG. 3 is a lens cross-sectional view illustrating a third configuration example of an imaging lens according to an embodiment of the present invention and corresponding to Example 3;

FIG. 4 is a lens cross-sectional view illustrating a fourth configuration example of an imaging lens according to an embodiment of the present invention and corresponding to Example 4;

FIG. 5 is a lens cross-sectional view illustrating a fifth configuration example of an imaging lens according to an embodiment of the present invention and corresponding to Example 5;

FIG. 6 is a lens cross-sectional view illustrating a sixth configuration example of an imaging lens according to an embodiment of the present invention and corresponding to Example 6;

FIG. 7 is a lens cross-sectional view illustrating a seventh configuration example of an imaging lens according to an embodiment of the present invention and corresponding to Example 7;

FIG. 8 is a lens cross-sectional view illustrating an eighth configuration example of an imaging lens according to an embodiment of the present invention and corresponding to Example 8;

FIG. 9 is a lens cross-sectional view illustrating a ninth configuration example of an imaging lens according to an embodiment of the present invention and corresponding to Example 9;

FIG. 10 is a lens cross-sectional view illustrating a tenth configuration example of an imaging lens according to an embodiment of the present invention and corresponding to Example 10;

FIG. 11 is a lens cross-sectional view illustrating an eleventh configuration example of an imaging lens according to an embodiment of the present invention and corresponding to Example 11;

FIG. 12 is an aberration diagram illustrating various aberrations of an imaging lens according to Example 1 of the present invention, where Section A shows a spherical aberration, Section B shows astigmatism (curvature of field), Section C shows distortion, and Section D shows a lateral chromatic aberration;

FIG. 13 is an aberration diagram illustrating various aberrations of an imaging lens according to Example 2 of the present invention, where Section A shows a spherical aberration, Section B shows astigmatism (curvature of field), Section C shows distortion, and Section D shows a lateral chromatic aberration;

FIG. 14 is an aberration diagram illustrating various aberrations of an imaging lens according to Example 3 of the present invention, where Section A shows a spherical aberration, Section B shows astigmatism (curvature of field), Section C shows distortion, and Section D shows a lateral chromatic aberration;

FIG. 15 is an aberration diagram illustrating various aberrations of an imaging lens according to Example 4 of the present invention, where Section A shows a spherical aberration, Section B shows astigmatism (curvature of field), Section C shows distortion, and Section D shows a lateral chromatic aberration;

FIG. 16 is an aberration diagram illustrating various aberrations of an imaging lens according to Example 5 of the present invention, where Section A shows a spherical aberration, Section B shows astigmatism (curvature of field), Section C shows distortion, and Section D shows a lateral chromatic aberration;

FIG. 17 is an aberration diagram illustrating various aberrations of an imaging lens according to Example 6 of the present invention, where Section A shows a spherical aberration, Section B shows astigmatism (curvature of field), Section C shows distortion, and Section D shows a lateral chromatic aberration;

FIG. 18 is an aberration diagram illustrating various aberrations of an imaging lens according to Example 7 of the present invention, where Section A shows a spherical aberration, Section B shows astigmatism (curvature of field), Section C shows distortion, and Section D shows a lateral chromatic aberration;

FIG. 19 is an aberration diagram illustrating various aberrations of an imaging lens according to Example 8 of the present invention, where Section A shows a spherical aberration, Section B shows astigmatism (curvature of field), Section C shows distortion, and Section D shows a lateral chromatic aberration;

FIG. 20 is an aberration diagram illustrating various aberrations of an imaging lens according to Example 9 of the present invention, where Section A shows a spherical aberration, Section B shows astigmatism (curvature of field), Section C shows distortion, and Section D shows a lateral chromatic aberration;

FIG. 21 is an aberration diagram illustrating various aberrations of an imaging lens according to Example 10 of the present invention, where Section A shows a spherical aberration, Section B shows astigmatism (curvature of field), Section C shows distortion, and Section D shows a lateral chromatic aberration;

FIG. 22 is an aberration diagram illustrating various aberrations of an imaging lens according to Example 11 of the present invention, where Section A shows a spherical aberration, Section B shows astigmatism (curvature of field), Section C shows distortion, and Section D shows a lateral chromatic aberration;

FIG. 23 is a diagram illustrating an imaging apparatus which is a cellular phone terminal including the imaging lens according to the present invention; and

FIG. 24 is a diagram illustrating an imaging apparatus which is a smartphone including the imaging lens according to the present invention.

DESCRIPTION OF THE PREFERRED EMBODIMENTS

Hereinafter, embodiments of the present invention will be described in detail with reference to the accompanying drawings.

FIG. 1 shows a first configuration example of an imaging lens according to a first embodiment of the present invention. The configuration example corresponds to a lens configuration of a first numerical value example (Table 1 and Table 2) to be described later. Likewise, FIGS. 2 to 11 show cross sections of second to eleventh configuration examples corresponding to the imaging lenses according to second to eleventh embodiments to be described later. The second to eleventh configuration examples correspond to lens configurations of the second to eleventh numerical value examples (Tables 3 to 22) to be described later. In FIGS. 1 to 11, the reference sign Ri represents a radius of curvature of i-th surface, where the number 35 i is the sequential number that sequentially increases as it gets closer to an image side (an imaging side) when a surface of a lens element closest to an object side is regarded as a first surface. The reference sign Di represents an on-axis surface spacing between i-th surface and (i+1) th surface on an optical axis Z1. Since the respective configuration examples are basically similar in configuration, the following description will be given on the basis of the first configuration example of the imaging lens shown in FIG. 1, and the configuration examples shown in FIGS. 2 to 11 will be also described as necessary. Further, FIGS. 1 to 11 also show the optical paths of on-axis rays 2 from the object point at an infinite distance, and rays 3 at the maximum angle of view.

An imaging lens L according to an embodiment of the present invention is appropriate to be used in various kinds of imaging apparatuses using imaging devices such as a CCD and a CMOS. Especially, the imaging lens L is appropriate to be used in relatively small-sized mobile terminal apparatus, for example, such as a digital still camera, a cellular phone with a camera, a smartphone, a tablet terminal, and a PDA. This imaging lens L includes, along the optical axis Z1, a first lens L1, a second lens L2, a third lens L3, a fourth lens L4, and a fifth lens L5 in this order from the object side.

FIG. 23 is a schematic diagram illustrating a cellular phone terminal, which is an imaging apparatus 1 according to an embodiment of the present invention. The imaging apparatus 1 according to the embodiment of the present invention includes imaging lens L according to the present embodiment and an imaging device 100 (refer to FIG. 1), such as a CCD, which outputs imaging signals based on an optical image formed by the imaging lens L. The imaging device 100 is disposed at an image formation surface (image plane R14) of the imaging lens L.

FIG. 24 is a schematic diagram illustrating a smartphone which is an imaging apparatus 501 according to an embodiment of the present invention. The imaging apparatus 501 according to the embodiment of the present invention includes a camera unit 541 including the imaging lens L according to the present embodiment and the imaging device 100 (refer to FIG. 1), such as a CCD, which outputs imaging signals based on an optical image formed by the imaging lens L. The imaging device 100 is disposed at the image formation surface (image plane R14) of the imaging lens L.

Various optical members CG may be disposed between the fifth lens L5 and the imaging device 100 based on the configuration of a camera on which the imaging lens is mounted. For example, a flat-plate-shaped optical member, such as a cover glass for protecting an imaging surface and an infrared-ray cut filter, may be disposed. In this case, for example, a flat-plate-shaped cover glass to which a coating having an effect of a filter, such as an infrared-ray cut filter and an ND filter, has been applied, or a material having the same effect may be used as the optical member CG.

Alternatively, an effect similar to the optical member CG may be given to the fifth lens L5 or the like by applying a coating to the fifth lens L5 or the like without using the optical member CG. Thereby, it is possible to reduce the number of components, and to reduce the total length.

Further, it is desirable that the imaging lens L includes an aperture stop St disposed on the object side of an object side surface of the second lens L2. Since the aperture stop St is disposed on the object side of the object side surface of the second lens L2 in such a manner, especially in a peripheral portion of an imaging area, it is possible to prevent an angle of incidence of rays, which pass through the optical system and are incident onto an imaging surface (imaging device), from becoming large. In order to further enhance this effect, it is more desirable that the aperture stop St be disposed on the object side of an object side surface of the first lens L1. Here, the expression “disposed on the object side of the object side surface of the second lens L2” means that the position of the aperture stop in the optical axis direction is the same as an intersection point between an on-axis marginal ray and the object side surface of the second lens L2 or located on the object side of the intersection point. Likewise, the expression “disposed on the object side of an object side surface of the first lens L1” means that the position of the aperture stop in the optical axis direction is the same as an intersection point between an on-axis marginal ray and the object side surface of the first lens L1 or located on the object side of the intersection point.

Furthermore, when the aperture stop St is disposed on the object side of the object side surface of the first lens L1 in the optical axis, it is desirable that the aperture stop St be disposed on the image side of a vertex of the surface of the first lens L1. When the aperture stop St is disposed on the image side of the vertex of the surface of the first lens L1 in such a manner, it is possible to reduce the total length of the imaging lens including the aperture stop St. The imaging lenses according to the first to seventh and tenth to eleventh embodiments (refer to FIGS. 1 to 7 and 10 to 11) are configuration examples in which the aperture stop St is disposed on the object side of the object side surface of the first lens L1, and the aperture stop St is disposed on the image side of the vertex of the surface of the first lens L1. However, the invention is not limited to the embodiments, and the aperture stop St may be disposed on the object side of the vertex of the surface of the first lens L1. The arrangement, in which the aperture stop St is disposed on the object side of the vertex of the surface of the first lens L1, is slightly disadvantageous in terms of securing a peripheral light amount, compared with a case where the aperture stop St is disposed on the image side of the vertex of the surface of the first lens L1. However, the arrangement can prevent an angle of incidence of rays, which pass through the optical system and are incident onto the imaging surface (imaging device), from becoming large in the peripheral portion of the imaging area in a more desirable manner. It should be noted that the aperture stop St shown herein does not necessarily represent the size or shape thereof but shows the position thereof on the optical axis Z1.

As in the imaging lenses according to the eighth and ninth embodiments shown in FIGS. 8 and 9, the aperture stop St may be disposed between the first lens L1 and the second lens L2 in the optical axis direction. In this case, it is possible to satisfactorily correct a curvature of field. When the aperture stop St is disposed between the first lens L1 and the second lens L2 in the optical axis direction, as compared with a case where the aperture stop St is disposed on the object side of the object side surface of the first lens L1 in the optical axis direction, this arrangement is disadvantageous in securing telecentricity, that is, making the principal rays parallel to such an extent that the principal rays are regarded as the optical axis (setting an incident angle thereof on the imaging surface such that the angle is approximate to zero). Thus, by applying an imaging device which is recently implemented as the development in the imaging device technology advances and in which deterioration in the light receiving efficiency and occurrence of color mixture due to increase of incident angle are more reduced than in the conventional imaging device, it is possible to achieve optimum optical performance.

In the imaging lens L, the first lens L1 has a positive refractive power, and has a meniscus shape which is concave toward the image side in the vicinity of the optical axis. By forming the first lens L1 in a meniscus shape which is concave toward the image side in the vicinity of the optical axis, the position of the rear side principal point of the first lens L1 can be set to be close to the object side, and thus it is possible to appropriately reduce the total length. Further, as shown in the first to eleventh embodiments, by forming the first lens L1 in an aspheric shape, it is possible to appropriately correct a spherical aberration.

The second lens L2 has a negative refractive power in the vicinity of the optical axis. Hence, it is possible to satisfactorily correct a spherical aberration and a longitudinal chromatic aberration which are caused when the rays pass through the first lens L1. Further, the second lens L2 may be concave toward the image side in the vicinity of the optical axis. In this case, since it is possible to satisfactorily correct a spherical aberration and a longitudinal chromatic aberration which are caused when the rays pass through the first lens L1, it is easy to reduce the total length. Further, as shown in the first, second, and sixth to tenth embodiments, the second lens L2 may have a biconcave shape in the vicinity of the optical axis. In this case, it is possible to suppress occurrence of a high-order spherical aberration while satisfactorily correcting a chromatic aberration. Further, as shown in the third and fourth embodiments, the second lens L2 may have a meniscus shape which is concave toward the image side in the vicinity of the optical axis. When the second lens L2 is formed in the meniscus shape which is concave toward the image side in the vicinity of the optical axis, the position of the rear side principal point of the second lens L2 can be set to be close to the object side, and thus it is possible to appropriately reduce the total length. Further, as shown in the fifth and eleventh examples, the second lens L2 may have a meniscus shape which is concave toward the object side in the vicinity of the optical axis. In this case, it is possible to suppress occurrence of astigmatism while satisfactorily correcting a chromatic aberration.

The third lens L3 has a negative refractive power. Further, it is desirable that an absolute value |f3| of the focal length of the third lens L3 be set to the maximum among absolute values |f1| to |f5| of the focal lengths of the first to fifth lenses L1 to L5. In this case, it is possible to more appropriately reduce an effect of change in a shape of the surface of the third lens L3 on the focal length f of the whole system, and thus the third lens L3 can be flexibly designed to have a shape of the surface appropriate for correcting various aberrations.

Further, it is desirable that the intersection point between the object side surface of the third lens L3 and the principal ray with the maximum angle of view be positioned on the object side of the intersection point between the object side surface of the third lens L3 and the optical axis. Thereby, compared with a case where the intersection point between the object side surface of the third lens L3 and the principal ray with the maximum angle of view is positioned on the image side of the intersection point between the object side surface of the third lens L3 and the optical axis, it is possible to further decrease the incident angle of the off-axis ray to the object side surface of the third lens L3, and thus it is possible to correct a spherical aberration with good balance while suppressing occurrence of astigmatism.

In order to further enhance the above effect, as shown in the first to eleventh embodiments, it is desirable that the intersection point between the object side surface of the third lens L3 and the principal ray with the maximum angle of view be positioned on the object side of the intersection point between the object side surface of the third lens L3 and the optical axis, and it is desirable that both surfaces of the third lens L3 have aspheric shapes. In this case, in accordance with an aberration such as a spherical aberration which occurs while the rays pass through the first lend L1 and the second lens L2 in the vicinity of the optical axis, the surface shape capable of appropriately correcting the aberration is appropriately selectable. Hence, it is possible to further correct a spherical aberration with good balance while suppressing occurrence of astigmatism. In addition, as shown the first to eighth embodiments and eleventh embodiment, the third lens L3 may have a meniscus shape which is convex toward the image side in the vicinity of the optical axis. When the third lens L3 has a meniscus shape which is convex toward the image side in the vicinity of the optical axis, it is possible to appropriately suppress occurrence of astigmatism. Further, as shown in the ninth and tenth embodiments, the third lens L3 may have a meniscus shape which is concave toward the image side in the vicinity of the optical axis. When the third lens L3 has a meniscus shape which is concave toward the image side in the vicinity of the optical axis, the position of the rear side principal point of the third lens L3 can be more appropriately set to be close to the object side, and thus it is possible to appropriately reduce the total length.

The fourth lens L4 has a positive refractive power in the vicinity of the optical axis. Further, it is desirable that the intersection point between the object side surface of the fourth lens L4 and the principal ray with the maximum angle of view be positioned on the object side of the intersection point between the object side surface of the fourth lens L4 and the optical axis. Thereby, compared with a case where the intersection point between the object side surface of the fourth lens L4 and the principal ray with the maximum angle of view is positioned on the image side of the intersection point between the object side surface of the fourth lens L4 and the optical axis, it is possible to further decrease the incident angle of the off-axis ray to the object side surface of the fourth lens L4, and thus it is possible to correct a spherical aberration with good balance while suppressing occurrence of astigmatism.

In order to further enhance the above effect, as shown in the first to eighth, tenth, and eleventh embodiments, it is desirable that the intersection point between the object side surface of the fourth lens L4 and the principal ray with the maximum angle of view be positioned on the object side of the intersection point between the object side surface of the fourth lens L4 and the optical axis, and it is desirable that both surfaces of the fourth lens L4 have aspheric shapes. In this case, in accordance with an aberration such as a spherical aberration which occurs while the rays pass through the first to third lenses L1 to L3 in the vicinity of the optical axis, the surface shape capable of appropriately correcting the aberration is appropriately selectable. Hence, it is possible to further correct a spherical aberration with good balance while suppressing occurrence of astigmatism. In addition, as shown in the seventh embodiment, the fourth lens L4 may have a meniscus shape which is concave toward the image side in the vicinity of the optical axis. In this case, it is possible to appropriately suppress occurrence of astigmatism. Further, as shown in the fifth and sixth embodiments, the fourth lens L4 may have a biconvex shape in the vicinity of the optical axis. In this case, it is possible to satisfactorily correct a spherical aberration. Further, as shown in the first to fourth embodiments and the eighth to eleventh embodiments, the fourth lens L4 may have a meniscus shape which is convex toward the image side in the vicinity of the optical axis. In this case, it is possible to appropriately suppress occurrence of astigmatism.

The fifth lens L5 has a negative refractive power in the vicinity of the optical axis. By making the fifth lens L5, which is disposed to be closest to the image plane side of the imaging lens, have a negative refractive power, it is possible to appropriately reduce the total length. Further, since the fifth lens L5 having a negative refractive power is disposed on the image side of the fourth lens L4 having a positive refractive power, it is possible to appropriately correct a lateral chromatic aberration and a curvature of field. Furthermore, as shown in the first, third, fourth, ninth, and eleventh embodiments, it is desirable that the fifth lens L5 have a biconcave shape in the vicinity of the optical axis. In this case, it is possible to adopt a configuration in which the fifth lens L5 has a desired negative refractive power without making the curvatures of both surfaces of the fifth lens L5 larger than necessary, and it is possible to appropriately reduce the total lens length while suppressing occurrence of various aberrations. In addition, as shown in the second, fifth to eighth, and tenth embodiments, the fifth lens L5 may have a meniscus shape which is convex toward the object side in the vicinity of the optical axis. In this case, it is possible to satisfactorily correct a curvature of field while more appropriately reducing the total length.

Further, the fifth lens L5 has an aspheric shape which has an extreme point on the image side surface. Thereby, it is possible to suppress an increase in distortion caused by the reduction in the total length, and it is possible to appropriately suppress various aberrations. The extreme point of the image side surface of the fifth lens L5 can be disposed at an arbitrary position inside of the intersection point between the image side surface of the fifth lens L5 and the principal ray with the maximum angle of view in the radial direction of the fifth lens L5.

It is further desirable that the fifth lens L5 have an aspheric shape which has an extreme point also on the object side surface. In this case, it is possible to more appropriately suppress an increase in distortion caused by the reduction in the total length, and it is possible to appropriately reduce various aberrations. The extreme point on the object side surface of the fifth lens L5 can be set at an arbitrary position outside the optical axis of the fifth lens L5 in the radial direction.

The imaging lenses according to the third, fourth, seventh, and eighth embodiments are configuration examples in which the fifth lens L5 has an extreme point on each of the image side surface and the object side surface. The imaging lenses according to the first, second, fifth, sixth, and ninth to eleventh embodiments are configuration examples in which the image side surface of the fifth lens L5 has an extreme point.

It should be noted that, in the present description, the “extreme point” means a point at which a function fx (r) is at a maximum value or a minimum value when a point on the lens surface within the effective diameter is represented by (r, fx (r)). Here, the distance from the optical axis in a direction perpendicular to the optical axis is r (r>0), and a function representing the position at the distance r in the optical axis direction is fx (r). All the extreme points of the respective embodiments of the present description are extreme points at which the tangent plane is perpendicular to the optical axis.

Further, the fifth lens L5 is concave toward the image side in the vicinity of the optical axis, and has an aspheric shape which has an extreme point on the image side surface. Hence, while obtaining an effect of reduction in the total length by applying the negative refractive power of the surface shape in the vicinity of the optical axis of the image side surface of the fifth lens L5, it is possible to suppress occurrence of distortion (distortion aberration) in a positive direction by applying the positive refractive power of the surface shape outside the extreme point of the image side surface of the fifth lens L5 in the radial direction.

Further, by making the fifth lens L5 concave toward the image side and making the image side surface of the fifth lens L5 have an aspheric shape which has at least one extreme point, especially in the peripheral portion of the imaging area, it is possible to prevent the angle of incidence of rays, which pass through the optical system and are incident onto the imaging surface (imaging device), from becoming large. It should be noted that the peripheral portion of the imaging area described herein means the outside of about 50% of the height in the radial direction. Here, the height is a height of the intersection point between the principal ray with the maximum angle of view and the surface from the optical axis.

According to the imaging lens L, in the imaging lens which is composed of five lenses as a whole, a configuration of each lens element of the first to fifth lenses L1 to L5 is optimized. Therefore, it is possible to achieve a lens system that has high resolution performance while decreasing the total length thereof.

In the imaging lens L, in order to enhance the performance thereof, it is desirable that at least one surface of each lens of the first to fifth lenses L1 to L5 be formed as an aspheric surface.

Further, it is desirable that each of the lenses L1 to L5 constituting the imaging lens L be not formed as a cemented lens but a single lens. The reason is that, compared with a case where any of the lenses L1 to L5 is formed as a cemented lens, since the number of aspheric surfaces increases, a degree of freedom in design of each lens is enhanced, and it is possible to appropriately achieve reduction in the total length thereof.

Further, for example, as in the imaging lenses according to the first to fifth embodiments, when each lens configuration of the first to fifth lenses L1 to L5 of the imaging lens L is set such that the total angle of view is equal to or greater than 50 degrees, the imaging lens L can be appropriately applied to a cellular phone terminal and the like which are often used in a close-up shot.

Next, effects and advantages of the conditional expressions of the imaging lens L configured as described above will be described in detail.

First, a focal length f of the whole system and a composite focal length f45 of the fourth and fifth lenses L4 and L5 satisfy the following conditional expression (1).

−1<f/f45<−0.105  (1)

The conditional expression (1) defines a desirable numerical range of a ratio of the focal length f of the whole system to the composite focal length f45 of the fourth and fifth lenses L4 and L5. By suppressing the negative composite refractive power of the fourth and fifth lenses L4 and L5 such that f/f45 is greater than the lower limit of the conditional expression (1), it is possible to satisfactorily correct astigmatism while suppressing occurrence of distortion in the positive direction. Further, by securing the negative composite refractive power of the fourth and fifth lenses L4 and L5 such that f/f45 is less than the upper limit of the conditional expression (1), there is an advantage in reducing the total length. In order to further enhance the effect, it is more desirable to satisfy the conditional expression (1-1), and it is even more desirable to satisfy the conditional expression (1-2).

−0.9<f/f45<−0.105  (1-1)

−0.8<f/f45<−0.1  (1-2)

Further, it is desirable that the thickness D6 of the third lens L3 on the optical axis and the focal length f of the whole system satisfy the following conditional expression (2).

0.02<D6/f<0.3  (2)

The conditional expression (2) defines a desirable range of a ratio of the thickness D6 of the third lens L3 on the optical axis to the focal length f of the whole system. By maintaining the thickness D6 of the third lens L3 on the optical axis such that D6/f is less than the upper limit of the conditional expression (2), it is possible to correct a spherical aberration with good balance while suppressing occurrence of astigmatism, and it is also possible to prevent the size of the imaging lens L from becoming large. By securing the thickness D6 of the third lens L3 on the optical axis such that D6/f is greater than the lower limit of the conditional expression (2), it is possible to suppress excessive reduction in the thickness D6 of the third lens L3 on the optical axis, and thus it is possible to correct a spherical aberration with good balance while suppressing occurrence of astigmatism. In order to further enhance the effect, it is more desirable to satisfy the conditional expression (2-1), and it is even more desirable to satisfy the conditional expression (2-2).

0.03<D6/f<0.2  (2-1)

0.04<D6/f<0.18  (2-2)

As described above, according to the imaging lens of the embodiment of the present invention, in the imaging lens which is composed of five lenses as a whole, the configuration of each lens element is optimized. Therefore, it is possible to achieve a lens system that has high resolution performance while decreasing the total length thereof.

The above imaging lens substantially consists of, in order from the object side: a first lens having a positive refractive power; a second lens having a negative refractive power; a third lens having a negative refractive power; a fourth lens having a positive refractive power; and a fifth lens having a negative refractive power. In addition, the imaging lens is composed of a first lens group, which includes the first to third lenses and has a positive refractive power, and a second lens group which includes the fourth lens and the fifth lens and has a negative refractive power. Hence, by making the whole imaging lens have a telephoto type configuration in which the first lens group having the positive refractive power and the second lens group having the negative refractive power are disposed in order from the object side, it is possible to appropriately reduce the total length. Further, in the imaging lens, by satisfying the conditional expression (1) and appropriately setting the refractive powers of the fourth lens L4 and the fifth lens L5, the effect of reduction in the total length is further enhanced. For example, assuming that the distance (the total length of the lens) on the optical axis from the object side surface of the first lens L1 to the image plane is L and the focal length of the whole system is f, in the first to eleventh embodiments, a telephoto ratio L/f, which indicates a ratio of the total lens length to the focal length f of the whole system, is about 0.868 to 1.116. In contrast, the lens system disclosed in Patent Document 1 (for example, refer to Example 11) employs a configuration similar to the lens configuration of the present invention, but in the lens system, the refractive power of the second lens group composed of the fourth lens and the fifth lens is not appropriately set, and thus the total lens length is not sufficiently reduced. For example, a telephoto ratio L/f of the lens system disclosed in Patent Document 1 is about 1.12, and a telephoto ratio of the lens system disclosed in Example 10 of Patent Document 2 is about 1.13.

By satisfying appropriately desirable conditions, it is possible to achieve higher imaging performance. Furthermore, according to the imaging apparatus of the embodiment, imaging signals based on an optical image, which is formed by the high-performance imaging lens according to the embodiment, are output. Therefore, it is possible to obtain a photographed image with high resolution in the range from the central angle of view to the peripheral angle of view.

Next, specific numerical examples of the imaging lens according to the embodiment of the present invention will be described. Hereinafter, a plurality of numerical examples will be described collectively.

Table 1 and Table 2, which will be given later, show specific lens data corresponding to the configuration of the imaging lens shown in FIG. 1. Specifically, Table 1 shows basic lens data, and Table 2 shows data on aspheric surfaces. In the lens data shown in Table 1, the column of surface number Si shows the surface number of the i-th surface in the imaging lens of Example 1. The surface of the lens element closest to the object side is the first surface (the aperture stop St is the first), and surface numbers sequentially increase toward the image side. The column of the radius of curvature Ri shows values (mm) of the radius of curvature of i-th surface from the object side to correspond to the reference sign Ri in FIG. 1. Likewise, the column of the on-axis surface spacing Di shows spaces (mm) on the optical axis between the i-th surface Si and the (i+1) th surface Si+1 on the optical axis from the object side. The column of Ndj shows values of the refractive index of the j-th optical element from the object side for the d-line (587.56 nm). The column of vdj shows values of the Abbe number of the j-th optical element from the object side for the d-line.

In the imaging lens according to Example 1, both surfaces of each of the first to fifth lenses L1 to L5 are aspheric. In the basic lens data shown in Table 1, the radii of curvature of these aspheric surfaces are represented as numerical values of the radius of curvature near the optical axis (paraxial radius of curvature).

Table 2 shows aspheric surface data in the imaging lens system according to Example 1. In the numerical values represented as the aspheric surface data, the reference sign “E” means that a numerical value following this is a “exponent” having a base of 10 and that this numerical value having a base of 10 and expressed by an exponential function is multiplied by a numerical value before the “E”. For example, this means that “1.0E-02” is “1.0×10⁻²”.

As aspheric surface data, values of coefficients Ai and KA in the aspheric surface expression represented by the following expression (A) are shown. Specifically, Z represents the length (mm) of a perpendicular from a point on an aspheric surface at height h from an optical axis to a plane that contacts with the vertex of the aspheric surface (the plane perpendicular to the optical axis).

Z=C·h ²/{1+(1−KA·C ² ·h ²)^(1/2) }+ΣAi·h ^(i)  (A)

Here,

Z is a depth of the aspheric surface (mm),

h is a distance (height) from the optical axis to the lens surface (mm),

C is a paraxial curvature=1/R

(R: a paraxial radius of curvature),

Ai is an i-th order aspheric surface coefficient (i is an integer equal to or greater than 3), and

KA is an aspheric surface coefficient.

As in the imaging lens according to the above-mentioned Example 1, Tables 3 to 22 show specific lens data as Examples 2 to 11, corresponding to the configuration of the imaging lenses shown in FIGS. 2 to 11. In the imaging lenses according to Examples 1 to 11, both surfaces of each of the first to fifth lenses L1 to L5 are aspheric.

FIG. 12, Section A to Section D show a spherical aberration, astigmatism (curvature of field), distortion (a distortion aberration), and a lateral chromatic aberration (a chromatic aberration of magnification) in the imaging lens of Example 1, respectively. Each aberration diagram illustrating a spherical aberration, astigmatism (curvature of field), and distortion (a distortion aberration) shows an aberration for the d-line (a wavelength of 587.56 nm) as a reference wavelength. The diagram of a spherical aberration diagram and the diagram of a lateral chromatic aberration diagram show also aberrations for the F-line (a wavelength of 486.1 nm) and the C-line (a wavelength of 656.27 nm). The diagram of a spherical aberration also shows an aberration for the g-line (a wavelength of 435.83 nm). In the diagram of astigmatism, the solid line indicates an aberration in the sagittal direction (S), and the broken line indicates an aberration in the tangential direction (T). Fno. indicates an F-number, and a) indicates a half angle of view.

Likewise, FIG. 13, Section A to D to FIG. 22, Section A to D show various aberrations of the imaging lenses of Examples 2 to 11.

Table 23 collectively shows values of the conditional expressions (1) and (2) of Examples 1 to 11 according to the present invention. In Table 23, Fno. is an F-number, f is the focal length of the whole system, Bf is a distance on the optical axis from the image side surface of the lens closest to the image side to the image plane (Bf corresponds to a back focal length), TL is a distance on the optical axis from the object side surface of the first lens L1 to the image plane, 2ω is a total angle of view, and f1 to f5 are the focal lengths of the first to fifth lenses L1 to L5, respectively. Bf is an air conversion length, that is, indicates a value which is calculated by air-converting the thickness of an optical member PP. Likewise, the back focal length portion of TL uses an air conversion length. As can be seen from Table 23, all Examples 1 to 11 satisfy the conditional expressions (1) and (2)

It should be noted that the respective tables show numerical values which are rounded off to a predetermined decimal place. Regarding units of the numerical values, “°” is used for an angle, and “mm” is used for a length. However, those are just examples, and other appropriate units may be used since the optical system has the same optical performance even when being scaled up or scaled down.

As can be seen from the above-mentioned numerical value data and aberration diagrams, in each example, high imaging performance is achieved while the total length is reduced.

The imaging lens of the present invention is not limited to the above-mentioned embodiments and examples, and may be modified to various forms. For example, the values of the radius of curvature, the on-axis surface spacing, the refractive index, the Abbe number, the aspheric surface coefficient, and the like of the lens elements are not limited to the values shown in the numerical examples, and may have different values.

Further, in the description of each of all the examples, it is a premise that the imaging lens is used with fixed focus, but it may be possible to adopt a configuration in which focus is adjustable. For example, the imaging lens may be configured in such a manner that autofocusing is possible by extending the whole lens system or by moving some lenses on the optical axis. Further, the imaging lens of the present invention may be configured such that, in each lens which is formed in a meniscus shape in the vicinity of the optical axis, a surface with a large absolute value of the radius of curvature of the meniscus shape in the vicinity of the optical axis is set to be planar. In other words, the lens, which is formed in a meniscus shape in the vicinity of the optical axis, may be a plano-convex lens or a plano-concave lens of which a surface with a large absolute value of the radius of curvature of the meniscus shape is planar.

TABLE 1 EXAMPLE 1 Si Ri Di Ndj νdj 1(APERTURE ∞ −0.334 STOP) *2 1.18899 0.571 1.54340 56.04 *3 99.65790 0.088 *4 −14.67650 0.200 1.63551 23.90 *5 3.01732 0.252 *6 −6.31497 0.597 1.63551 23.90 *7 −6.65299 0.411 *8 −1.81343 0.300 1.54340 56.04 *9 −1.31209 0.681 *10  −44.87922 0.200 1.54340 56.04 *11  2.04691 0.500 12 ∞ 0.300 1.51680 64.20 13 ∞ 0.304 14 ∞ *ASPHERIC SURFACE

TABLE 2 EXAMPLE 1 • ASPHERIC SURFACE DATA SURFACE NUMBER KA A4 A6 A8 A10 1 −3.0731906E+00 3.0454133E−01 −1.5990384E−01   1.7247286E−01 −5.3178441E−02 3 −9.1399077E+00 4.0884605E−02 7.1663951E−02 −1.6539850E−01  2.8153214E−01 4 −7.7325444E+00 1.0926734E−01 4.1997100E−02  2.0010795E−01 −7.2997830E−01 5  7.3972620E+00 5.0503278E−02 2.0519314E−01  3.4434102E−02 −2.9379200E−01 6 −2.7252706E+00 −1.8102233E−01  −3.0449414E−02   2.8735459E−01 −4.7439132E−01 7 −9.4797096E+00 −1.0159680E−01  −3.8584449E−02   1.3304889E−01 −5.5892757E−02 8  5.8027401E−01 3.2649400E−02 3.5012275E−02 −1.6276124E−01  2.0346862E−01 9 −1.9393751E+00 5.8819137E−02 6.0098782E−02 −7.6772582E−02  3.8460773E−02 10  8.2201964E+00 −6.9397631E−02  3.5778296E−02 −1.0729204E−02  2.1484330E−03 11 −9.9999986E+00 −8.4004663E−02  3.4511556E−02 −1.0919218E−02  2.1061098E−03 A12 A14 2 −2.2766050E−02 4.8223278E−02 3 −3.5115313E−01 1.9300135E−01 4  8.3838365E−01 −2.8308539E−01  5  4.0531854E−01 8.3857848E−01 6  1.4101685E−01 0.0000000E+00 7  1.5928690E−02 0.0000000E+00 8 −9.7182313E−02 1.7144587E−02 9 −9.4639185E−03 8.2664368E−04 10 −2.4392660E−04 1.1524539E−05 11 −2.1868938E−04 9.5754576E−06

TABLE 3 EXAMPLE 2 Si Ri Di Ndj νdj 1(APERTURE ∞ −0.329 STOP) *2 1.13267 0.598 1.54340 56.04 *3 261.35856 0.058 *4 −24.28652 0.200 1.63551 23.90 *5 3.08695 0.249 *6 −4.71522 0.710 1.63551 23.90 *7 −5.40306 0.277 *8 −1.46920 0.342 1.54340 56.04 *9 −1.36496 0.558 *10  31.17972 0.312 1.54340 56.04 *11  2.22683 0.500 12 ∞ 0.300 1.51680 64.20 13 ∞ 0.299 14 ∞ *ASPHERIC SURFACE

TABLE 4 EXAMPLE 2 • ASPHERIC SURFACE DATA SURFACE NUMBER KA A4 A6 A8 A10 2 −2.8039625E+00 3.2419356E−01 −1.5263307E−01   1.7557493E−01 −4.0496896E−02 3 −1.8439549E+00 6.7036389E−02 6.3669727E−02 −1.7213129E−01  1.9725783E−01 4 −9.8171198E+00 1.5166971E−01 8.9169351E−03  1.3902602E−01 −7.1105789E−01 5  7.1695083E+00 1.1110231E−01 2.1270293E−01  5.7907570E−03 −3.4191808E−01 6 −4.7791782E+00 −1.0704893E−01  −4.3433343E−02   2.1641744E−01 −2.6261512E−01 7 −9.2275791E+00 −4.1792103E−02  −3.6285513E−02   1.3643041E−01 −5.4657167E−02 8  4.0346898E−01 2.2771633E−02 4.5548573E−02 −1.5725047E−01  2.0386033E−01 9 −2.0251511E+00 4.7820241E−02 5.3515218E−02 −7.7167322E−02  3.9134775E−02 10 −9.9984367E+00 −7.0612037E−02  3.5601421E−02 −1.0770954E−02  2.1452429E−03 11 −9.9999986E+00 −8.4541891E−02  3.4821211E−02 −1.0955812E−02  2.1033674E−03 A12 A14 2 −1.9482308E−02 3.3120131E−02 3 −3.5480500E−01 3.2643492E−01 4  8.0972407E−01 −2.3243392E−02  5  3.1246773E−01 2.2094920E+00 6 −5.6542589E−01 0.0000000E+00 7  1.0719305E−03 0.0000000E+00 8 −9.9158165E−02 2.5065669E−02 9 −9.2206177E−03 7.0112394E−04 10 −2.4378785E−04 1.1627667E−05 11 −2.1903636E−04 9.4020312E−06

TABLE 5 EXAMPLE 3 Si Ri Di Ndj νdj 1(APERTURE ∞ −0.351 STOP) *2 1.16356 0.508 1.54400 55.90 *3 12.77653 0.053 *4 8.36630 0.200 1.63400 23.80 *5 1.86361 0.482 *6 −9.71630 0.215 1.63400 23.80 *7 −9.94789 0.621 *8 −15.85010 0.365 1.54400 55.90 *9 −0.92052 0.166 *10  −1.09965 0.200 1.54400 55.90 *11  3.19024 0.500 12 ∞ 0.300 1.51700 64.20 13 ∞ 0.601 14 ∞ *ASPHERIC SURFACE

TABLE 6 EXAMPLE 3—ASPHERIC SURFACE DATA SURFACE NUMBER KA A4 A6 A8 A10 2 −2.6145923E+00   2.7924291E−01 −5.5785213E−02 −7.5850758E−02   1.5387567E−01 3 −4.0627471E+03 −1.5151510E−02   8.5990937E−02   1.9749686E−02   7.2639462E−02 4 −1.0541664E+03 −7.8443143E−02   4.1577200E−01 −2.0934775E−01 −4.2990276E−01 5   5.4400320E+00 −1.4568637E−01   5.5313900E−01 −7.7122315E−01   5.4450400E−01 6   9.6526194E+00 −2.8952538E−01 −6.0869535E−02   2.9148312E−01   1.6556166E−01 7   4.5848148E+01 −2.8550165E−01   8.4803519E−02 −2.1646586E−02   1.8581169E−01 8   3.9075266E+01 −1.1173461E−01   7.3297460E−03 −4.7749954E−02   3.3505509E−02 9 −3.2952895E+00   2.7084846E−02   2.6162253E−02 −2.9561382E−02   7.5720451E−03 10 −5.4482134E+00   3.1927750E−02 −7.4650758E−03   1.6950727E−03 −1.2148648E−04 11 −5.6444979E+01 −6.1131740E−02   6.3802384E−03 −1.8227098E−03   5.2387716E−04 A12 A14 2   7.8745435E−02 −1.0903667E−01 3 −1.9649917E−01   1.3878199E−02 4   7.7773677E−01 −5.2976854E−01 5   3.2619409E−01 −8.6573255E−01 6 −6.4690724E−02 −2.1180539E−01 7   1.6846583E−01 −2.2288715E−01 8   7.9572918E−04 −2.2633586E−03 9   1.3317611E−04 −1.8863793E−04 10   3.1654130E−06   7.1151479E−07 11 −5.7791200E−06 −6.5142877E−07

TABLE 7 EXAMPLE 4 Si Ri Di Ndj νdj  1 ∞ −0.351 (APERTURE STOP)  *2 1.16701 0.496 1.54400 55.90  *3 12.00739 0.050  *4 6.02463 0.200 1.63400 23.80  *5 1.97699 0.483  *6 −3.94924 0.267 1.63400 23.80  *7 −4.07809 0.645  *8 −10.78573 0.455 1.54400 55.90  *9 −0.77511 0.136 *10 −0.88862 0.200 1.54400 55.90 *11 2.63278 0.500  12 ∞ 0.300 1.51700 64.20  13 ∞ 0.601  14 ∞ *ASPHERIC SURFACE

TABLE 8 EXAMPLE 4 • ASPHERIC SURFACE DATA SURFACE NUMBER KA A4 A6 A8 A10 2 −2.6767504E+00 2.8222995E−01 −5.3230549E−02 −7.5814482E−02 1.5924833E−01 3 −3.6123105E+03 −6.6797265E−03 7.2024243E−02 1.4490583E−02 9.2831597E−02 4 −8.4576581E+02 −7.9001433E−02 4.1828122E−01 −2.3921311E−01 −4.1584367E−01 5 6.1626196E+00 −1.4491250E−01 5.4636322E−01 −7.9594608E−01 5.9273153E−01 6 −7.3576491E+00 −2.5499140E−01 −4.7165163E−02 3.1192082E−01 1.6564220E−01 7 9.7081433E+00 −2.0659701E−01 9.4127345E−02 −2.1260698E−02 1.9014426E−01 8 1.6017132E+01 −1.1256500E−01 8.3718725E−03 −4.7825639E−02 3.3475189E−02 9 −3.7278467E+00 2.1786245E−02 2.7092786E−02 −2.9398633E−02 7.5856118E−03 10  −5.4294121E+00 2.9284483E−02 −7.2182817E−03 1.6936087E−03 −1.2648379E−04 11  −5.8601501E+01 −6.2512726E−02 5.8399804E−03 −1.8339710E−03 5.2202163E−04 A12 A14 A16 2 7.3615719E−02 −1.0522432E−01 0.0000000E+00 3 −1.8839234E−01 8.9319170E−03 0.0000000E+00 4 9.1046598E−01 −6.3327129E−01 0.0000000E+00 5 4.4092676E−01 −8.0888135E−01 0.0000000E+00 6 −8.3320146E−02 −1.9301756E−01 0.0000000E+00 7 1.7063447E−01 −2.2742547E−01 0.0000000E+00 8 8.1327944E−04 −2.2493429E−03 0.0000000E+00 9 1.3395918E−04 −1.8995065E−04 0.0000000E+00 10  1.9485009E−06 5.9102402E−07 0.0000000E+00 11  −7.1516507E−06 −1.0914416E−06 0.0000000E+00

TABLE 9 EXAMPLE 5 Si Ri Di Ndj νdj  1 ∞ −0.051 (APERTURE STOP) *2 1.49515 0.528 1.52999 56.56 *3 60.77184 0.199 *4 −4.84638 0.357 1.62053 23.49 *5 −43.29513 0.699 *6 −2.99319 0.434 1.59391 49.91 *7 −6.53278 0.507 *8 50.46015 0.408 1.63400 23.46 *9 −7.51004 0.408 *10  593.76473 0.923 1.53001 56.22 *11  2.08206 0.490 12 ∞ 0.210 1.51633 64.14 13 ∞ 0.260 14 ∞ *ASPHERIC SURFACE

TABLE 10 EXAMPLE 5 • ASPHERIC SURFACE DATA SURFACE NUMBER KA A3 A4 A5 A6 2 −2.0389432E+01 0.0000000E+00 −1.0267663E−01 1.7897563E+01 −1.5158801E+02 3 −2.3463409E+01 0.0000000E+00 −3.9041210E−01 4.0052266E+00 −2.1148635E+01 4 −1.6964387E+01 0.0000000E+00 −2.2175122E−01 3.3423785E+00 −1.7454682E+01 5 −1.0000090E+00 0.0000000E+00 5.6854527E−01 −3.4226924E+00 1.0402560E+01 6 −2.5208594E+01 0.0000000E+00 7.8860175E−02 4.7868189E−01 −7.5572534E+00 7 −9.6721497E+00 0.0000000E+00 3.4790043E−01 −9.8298115E−01 −2.5860640E−01 8 −1.0000090E+00 0.0000000E+00 1.5584533E+00 −5.1194578E+00 8.3678644E+00 9 1.0000738E+00 0.0000000E+00 2.7189080E+00 −1.0777028E+01 2.3377037E+01 10  −6.0939090E+00 0.0000000E+00 1.7935727E+00 −7.1108136E+00 1.1171314E+01 11  −4.4701750E+00 0.0000000E+00 3.3246433E−01 −1.6285435E+00 2.2207558E+00 A7 A8 A9 A10 A11 2 6.6286415E+02 −1.6976750E+03 2.4194257E+03 −1.2223569E+03 −1.3828394E+03 3 6.2289021E+01 −9.4538981E+01 2.5529698E+01 1.3316391E+02 −1.4192396E+02 4 5.0919604E+01 −8.9729985E+01 1.2285240E+02 −2.2875514E+02 4.5505375E+02 5 −1.1133571E+01 2.1500607E+01 −2.2710694E+02 9.1107123E+02 −1.8285964E+03 6 2.0822296E+01 −2.6658282E+01 2.8305679E+01 −4.7548393E+01 5.9054836E+01 7 4.6994403E+00 −1.2069102E+01 1.6303110E+01 −6.7045527E+00 −1.0690993E+01 8 −5.1432685E+00 −7.3674345E+00 1.5742200E+01 −7.0947737E+00 −6.2743200E+00 9 −3.1810995E+01 2.5731143E+01 −9.6217351E+00 −1.8332456E+00 3.7127490E+00 10  −7.9572204E+00 4.5223696E−01 3.4692255E+00 −2.7055463E+00 1.0735499E+00 11  −1.1847462E+00 −9.6421125E−02 4.1762268E−01 −1.4875831E−01 −3.5185903E−02 A12 A13 A14 A15 A16 2 1.8260521E+03 1.0723277E+03 −3.3053621E+03 2.3423952E+03 −5.8111471E+02 3 −1.1347952E+02 3.2141734E+02 −2.3939069E+02 6.6971227E+01 −2.6703722E+00 4 −5.3679205E+02 2.1209090E+02 1.9053377E+02 −2.3237645E+02 7.0636574E+01 5 2.0581302E+03 −1.2579251E+03 3.0914362E+02 4.7146969E+01 −2.9547676E+01 6 −1.8828966E+01 −3.5248371E+01 4.2435823E+01 −1.8290064E+01 2.8466940E+00 7 1.4065130E+01 −2.5050978E+00 −4.9360364E+00 3.3044009E+00 −6.4158617E−01 8 7.3922937E+00 −9.2086714E−01 −1.9938065E+00 1.0908279E+00 −1.7764775E−01 9 −1.8038088E+00 5.5403288E−01 −1.7220626E−01 4.7747960E−02 −6.1655701E−03 10  −3.3573962E−01 1.1700521E−01 −3.4085774E−02 5.3854310E−03 −3.0259102E−04 11  3.5722896E−02 −4.6193567E−03 −2.6225916E−03 9.5957509E−04 −9.4718795E−05

TABLE 11 EXAMPLE 6 Si Ri Di Ndj νdj  1 ∞ −0.150 (APERTURE STOP) *2 1.58500 0.605 1.53410 55.80 *3 207.46690 0.188 *4 −7.22216 0.357 1.63370 24.10 *5 13.70011 0.325 *6 −6.52435 0.367 1.53372 55.82 *7 −7.26771 0.480 *8 39.46237 0.453 1.63164 21.50 *9 −65.97414 0.161 *10  3.22391 0.914 1.53390 55.95 *11  1.64413 0.487 12 ∞ 0.145 1.51633 64.14 13 ∞ 0.490 14 ∞ *ASPHERIC SURFACE

TABLE 12 EXAMPLE 6 • ASPHERIC SURFACE DATA SURFACE NUMBER KA A3 A4 A5 A6 2 −1.9604024E+01 −2.7410492E−02 −5.5042233E−01 2.3211271E+01 −1.8433927E+02 3 −4.4721653E+01 −7.8305041E−04 −1.9705229E−01 1.4241934E+00 −5.4647287E+00 4 −4.4786849E+00 9.2169775E−03 −3.6438354E−02 4.8573753E−01 −2.2220869E+00 5 1.1874999E+01 −3.8933689E−03 −4.5014117E−03 9.8878294E−01 −4.2118569E+00 6 2.4960353E+00 2.3895654E−02 −1.1822186E−02 −1.0530811E+00 1.6746807E+00 7 7.8919147E+00 2.5612849E−02 5.4516362E−01 −6.0652408E+00 2.4541609E+01 8 −8.0561296E+00 3.3411384E−03 1.4049366E+00 −9.4367823E+00 3.3382451E+01 9 1.0000096E+00 −1.6466850E−02 1.1610633E+00 −4.5149064E+00 9.0738246E+00 10  −4.7876367E+00 −1.7251991E−02 4.3909478E−01 −2.3697397E+00 4.2678462E+00 11  −3.1795528E+00 −2.5540757E−02 1.8112566E−01 −1.1718884E+00 2.3154327E+00 A7 A8 A9 A10 A11 2 7.5278917E+02 −1.6572950E+03 1.4239078E+03 1.6368233E+03 −4.8119348E+03 3 3.0650226E+00 4.6534584E+01 −1.7722059E+02 2.8158305E+02 −1.4996673E+02 4 6.1717221E+00 −1.0182726E+01 8.5310651E+00 −2.5016451E+00 5.6297775E+00 5 6.4279781E+00 6.9975562E+00 −3.1491105E+01 8.8309805E+00 7.3140592E+01 6 9.2179979E+00 −4.9084879E+01 9.2066584E+01 −6.3237674E+01 −1.4583154E+01 7 −5.6460819E+01 7.6901421E+01 −5.7531093E−01 9.6852795E+00 3.0016752E+01 8 −6.9275009E+01 8.4866217E+01 −5.5326366E+01 6.6670909E+00 1.6593138E+01 9 −1.0330993E+01 5.7768192E+00 −1.6141589E−01 −1.5637535E+00 5.4743138E−01 10  −4.1767348E+00 2.3361707E+00 −7.5847935E−01 3.1869462E−01 −3.3107160E−01 11  −2.3304941E+00 1.0976669E+00 6.3261420E−02 −3.3465382E−01 1.2662735E−01 A12 A13 A14 A15 A16 2 1.9493142E+03 5.9156555E+03 −9.4335012E+03 5.6779926E+03 −1.2922165E+03 3 −1.7095144E+02 3.3731101E+02 −2.3140512E+02 7.6924136E+01 −1.1902385E+01 4 −2.2544253E+01 4.0438718E+01 −4.7471782E+01 3.5639281E+01 −1.1993528E+01 5 −8.6342467E+01 −2.3427266E+01 9.8606678E+01 −6.0442645E+01 1.1063294E+01 6 −3.2250039E−01 9.5456363E+01 −1.0610765E+02 3.7068329E+01 −1.2077524E+00 7 −4.5231523E+01 4.0170861E+01 −2.3661316E+01 8.1842458E+00 −1.2357787E+00 8 −1.0343947E+01 −3.3813030E−03 2.2549693E+00 −8.9331312E−01 1.1484796E−01 9 2.2412782E−01 −2.0658849E−01 5.3568831E−02 −4.3753786E−03 −1.3294129E−04 10  2.4702921E−01 −1.0721097E−01 2.7567804E−02 −3.9621477E−03 2.4712672E−04 11  1.9333360E−02 −3.0221675E−02 1.0307768E−02 −1.6132406E−03 1.0024024E−04

TABLE 13 EXAMPLE 7 Si Ri Di Ndj νdj  1 ∞ −0.150 (APERTURE STOP) *2 1.57461 0.603 1.53410 55.80 *3 47.79241 0.188 *4 −7.12102 0.348 1.63370 24.10 *5 19.52526 0.343 *6 −6.42339 0.383 1.53372 55.82 *7 −8.05667 0.480 *8 25.81378 0.403 1.63164 21.50 *9 47.55690 0.157 *10  3.09120 0.967 1.53390 55.95 *11  1.73973 0.487 12 ∞ 0.145 1.51633 64.14 13 ∞ 0.469 14 ∞ *ASPHERIC SURFACE

TABLE 14 EXAMPLE 7 • ASPHERIC SURFACE DATA SURFACE NUMBER KA A3 A4 A5 A6 2 −2.0107696E+01 −2.2661782E−02 −5.4399900E−01 2.3217910E+01 −1.8438211E+02 3 −4.4357390E+01 −2.5497459E−03 −1.9583400E−01 1.4073340E+00 −5.4400771E+00 4 −9.0798016E+00 1.0956079E−02 −5.3381786E−02 4.9837678E−01 −2.2074690E+00 5 −6.9683630E+01 −7.4427956E−03 −2.9622375E−03 9.9809263E−01 −4.2153635E+00 6 −2.3338456E+01 1.4097596E−02 −2.4009851E−02 −1.0521517E+00 1.6716424E+00 7 −7.8920388E+00 1.3735682E−02 5.5837573E−01 −6.0827370E+00 2.4539937E+01 8 −8.3236335E+00 2.2299801E−03 1.4226945E+00 −9.4489784E+00 3.3378436E+01 9 1.0000090E+00 −8.6603973E−03 1.1455767E+00 −4.5122894E+00 9.0734474E+00 10  −7.4372006E+00 4.6403018E−04 4.2832804E−01 −2.3674084E+00 4.2680533E+00 11  −5.5796708E+00 6.4774038E−03 1.8274058E−01 −1.1766013E+00 2.3152449E+00 A7 A8 A9 A10 A11 2 7.5279492E+02 −1.6572634E+03 1.4239324E+03 1.6368217E+03 −4.8119636E+03 3 3.0578468E+00 4.6535099E+01 −1.7723702E+02 2.8157926E+02 −1.4995313E+02 4 6.1772685E+00 −1.0198525E+01 8.5190124E+00 −2.4989492E+00 5.6335613E+00 5 6.4279893E+00 6.9983127E+00 −3.1478770E+01 8.8335446E+00 7.3148008E+01 6 9.2198343E+00 −4.9079113E+01 9.2056443E+01 −6.3240981E+01 −1.4591993E+01 7 −5.6459991E+01 7.6904242E+01 −5.7529617E+01 9.6838070E+00 3.0016274E+01 8 −6.9274235E+01 8.4867452E+01 −5.5326384E+01 6.6669423E+00 1.6593071E+01 9 −1.0331082E+01 5.7768697E+00 −1.6138063E−01 −1.5637188E+00 5.4745230E−01 10  −4.1767785E+00 2.3361604E+00 −7.5848276E−01 3.1869381E−01 −3.3107200E−01 11  −2.3303741E+00 1.0976932E+00 6.3266721E−02 −3.3465302E−01 1.2662733E−01 A12 A13 A14 A15 A16 2 1.9492888E+03 5.9156569E+03 −9.4334918E+03 5.6780045E+03 −1.2922192E+03 3 −1.7096360E+02 3.3733896E+02 −2.3138028E+02 7.6916678E+01 −1.1947535E+01 4 −2.2539556E+01 4.0469790E+01 −4.7487679E+01 3.5627556E+01 −1.2004892E+01 5 −8.6353096E+01 −2.3435645E+01 9.8594183E+01 −6.0445865E+01 1.1081962E+01 6 −3.2390099E−01 9.5463391E+01 −1.0609281E+02 3.7057311E+01 −1.2057907E+00 7 −4.5233308E+01 4.0168803E+01 −2.3662403E+01 8.1846925E+00 −1.2338297E+00 8 −1.0343985E+01 −3.3639720E−03 2.2549613E+00 −8.9330563E−01 1.1484978E−01 9 2.2413434E−01 −2.0658978E−01 5.3566530E−02 −4.3764378E−03 −1.3278690E−04 10  2.4702924E−01 −1.0721095E−01 2.7567808E−02 −3.9621449E−03 2.4712851E−04 11  1.9333441E−02 −3.0221675E−02 1.0307763E−02 −1.6132445E−03 1.0023928E−04

TABLE 15 EXAMPLE 8 Si Ri Di Ndj νdj *1 1.56927 0.612 1.53410 55.80 *2 62.77589 0.126  3 ∞ 0.063 (APERTURE STOP) *4 −6.30119 0.354 1.63370 24.10 *5 31.24436 0.328 *6 −6.33840 0.349 1.53372 55.82 *7 −7.46913 0.463 *8 −62.84123 0.380 1.63164 21.50 *9 −29.03855 0.176 *10  2.99641 0.938 1.53390 55.95 *11  1.62519 0.487 12 ∞ 0.145 1.51633 64.14 13 ∞ 0.484 14 ∞ *ASPHERIC SURFACE

TABLE 16 EXAMPLE 8 • ASPHERIC SURFACE DATA SURFACE NUMBER KA A3 A4 A5 A6 1 −1.9498259E+01 0.0000000E+00 −1.2678403E−01 7.4463227E+00 −2.4961395E+01 2 3.6086370E+00 0.0000000E+00 −2.7274111E−01 2.2441876E+00 −1.0662053E+01 4 −5.0253863E+00 0.0000000E+00 1.5158641E−01 −1.6580576E+00 9.6834090E+00 5 1.0740752E+01 0.0000000E+00 −1.2937718E−01 2.2130863E+00 −9.6919780E+00 6 2.7788659E+00 0.0000000E+00 9.1677765E−01 −9.6947664E+00 4.2266864E+01 7 6.9209073E+00 0.0000000E+00 1.4597058E+00 −1.1896778E+01 4.0075788E+01 8 −8.3649266E+00 0.0000000E+00 1.7195168E+00 −9.2047912E+00 2.5189628E+01 9 9.6225742E−01 0.0000000E+00 1.1958066E+00 −3.5480021E+00 2.8447742E+00 10  −7.4372609E+00 0.0000000E+00 5.5822003E−01 −2.8952257E+00 5.3221412E+00 11  −2.5143090E+00 0.0000000E+00 −1.3376055E−01 −4.6783336E−02 2.5148559E−01 A7 A8 A9 A10 A11 1 −4.7840875E+01 5.4833738E+02 −1.5505225E+03 1.6629091E+03 7.6876452E+02 2 2.4106664E+01 −1.0102384E+01 −8.4860045E+01 2.5455188E+02 −4.5305500E+02 4 −1.9875368E+01 −5.3708956E+01 3.8494739E+02 −7.4935411E+02 2.2561769E+02 5 1.6859111E+01 1.1622654E+01 −7.5229001E+01 1.3193842E+01 2.2456527E+02 6 −9.5097621E+01 7.7581678E+01 9.6831074E+01 −2.0965999E+02 −8.5394699E+01 7 −6.2048443E+01 6.9035575E+00 1.1799100E+02 −1.5103559E+02 5.2703168E+01 8 −3.7190405E+01 2.5025731E+01 4.8009978E−01 −6.5439415E+00 −4.9331564E+00 9 6.6003076E+00 −1.9749997E+01 2.2323831E+01 −1.2567009E+01 2.9805026E+00 10  −5.2991216E+00 2.8346627E+00 −5.9189414E−01 1.7428946E−02 −2.0557568E−01 11  −2.3239759E−01 7.0762172E−02 −2.4029042E−03 3.3980208E−02 −4.1691366E−02 A12 A13 A14 A15 A16 1 −3.3843753E+03 1.7707007E+03 1.6269970E+03 −6.0197204E+02 −2.7643785E+03 2 6.7019959E+02 −6.4964530E+02 −9.6481880E+01 1.2277909E+03 −1.5538838E+03 4 5.7142615E+02 2.1132168E+03 −7.8700807E+03 7.3789144E+03 1.4951146E+03 5 −6.9246658E+01 −8.5684519E+02 1.3114538E+03 −7.5231584E+01 −1.4016346E+03 6 4.7057506E+02 −2.2678882E+02 −3.9177203E+02 4.7952635E+02 −8.8872307E+01 7 −5.1746545E+01 1.9288276E+02 −1.9159410E+02 4.2534695E−01 1.1228879E+02 8 6.1266756E+00 3.2017468E+00 −5.7426214E+00 1.5294774E+00 8.4828869E−01 9 8.7228059E−02 −3.4439816E−01 6.4828115E−01 −6.6768225E−01 3.2879472E−01 10  2.2559541E−01 −8.9556500E−02 9.5654337E−03 3.3868106E−03 −9.0019404E−04 11  1.4802969E−02 1.4547836E−03 −2.0984112E−03 2.5706385E−04 1.1960968E−04 A17 A18 1 2.8028209E+03 −8.1398936E+02 2 8.7454032E+02 −1.9478922E+02 4 −6.2441064E+03 2.7849394E+03 5 1.2767488E+03 −3.6879271E+02 6 −1.0613015E+02 4.5609491E+01 7 −7.0736402E+01 1.4217356E+01 8 −5.5427310E−01 8.8823273E−02 9 −7.8924948E−02 7.5382746E−03 10  −1.5910886E−05 1.5942007E−05 11  −3.8181629E−05 3.2282100E−06

TABLE 17 EXAMPLE 9 Si Ri Di Ndj νdj *1 1.12444 0.546 1.54488 54.87 *2 252.97534 0.030  3 ∞ 0.069 (APERTURE STOP) *4 −18.78836 0.227 1.63351 23.63 *5 2.25616 0.243 *6 506.45581 0.253 1.63351 23.63 *7 4.36560 0.506 *8 −99.83715 0.506 1.63351 23.63 *9 −1.70702 0.100 *10  −2.17464 0.253 1.54488 54.87 *11  3.61429 0.500 12 ∞ 0.300 1.51633 64.14 13 ∞ 1.740 14 ∞ *ASPHERIC SURFACE

TABLE 18 EXAMPLE 9 • ASPHERIC SURFACE DATA SURFACE NUMBER KA A4 A6 A8 A10 1 6.9377302E−01 −8.6315370E−03 −2.9322827E−03 −2.8236519E−01 3.6582042E−01 2 1.0000090E+00 1.0299728E−02 −3.3338883E−02 −3.5854402E−01 −2.1599412E−01 4 9.8073731E+00 4.1860316E−01 2.4161475E−01 −7.6083670E−01 −7.7068397E−01 5 3.1182039E+00 4.6995645E−01 1.5149631E+00 −2.7101440E+00 1.3698992E+01 6 6.1881621E−01 −1.9777356E−01 1.5104859E+00 −1.5044509E+00 1.4799995E+00 7 9.9999979E−01 −1.3815608E−01 8.2457564E−01 −4.9516542E−01 2.3119410E+00 8 3.2258104E−01 −7.2840681E−02 1.5663313E−01 9.8367802E−02 −2.7569022E−01 9 −2.6292010E+00 1.1379689E−01 −1.7291781E−02 2.9845655E−02 1.7970251E−04 10  −1.4000002E+01 −4.4092972E−02 9.9278653E−02 −7.7922450E−02 2.0967820E−02 11  1.3000586E−01 −1.8315230E−01 1.3758774E−01 −9.0542240E−02 4.2054637E−02 A12 A14 A16 1 −4.2487703E−01 −2.2631039E−01 −2.0344291E−02 2 −4.4977846E−01 2.5600140E+00 −1.9687116E+00 4 2.7743135E−01 2.0383002E+00 7.4259109E−01 5 −3.8132984E+01 5.1107685E+01 −2.7851932E+01 6 1.8815842E+01 −1.1654772E+02 1.7961509E+02 7 −1.5309306E+01 2.6135941E+01 −1.0762516E+01 8 1.7783105E−01 −4.9261478E−02 3.9419268E−03 9 −2.1611961E−02 4.0098433E−03 1.4790761E−03 10  4.6775947E−03 −9.1757326E−04 −4.2752923E−04 11  −1.3115957E−02 2.7031329E−03 −1.9876871E−04

TABLE 19 EXAMPLE 10 Si Ri Di Ndj νdj  1 ∞ −0.278 (APERTURE STOP) *2 1.17174 0.557 1.54488 54.87 *3 101.21828 0.101 *4 −8.52605 0.334 1.63351 23.63 *5 3.10246 0.243 *6 253.12530 0.354 1.54488 54.87 *7 7.08468 0.350 *8 −4.62732 0.427 1.63351 23.63 *9 −2.28837 0.246 *10  2.81503 0.351 1.63351 23.63 *11  1.45940 0.500 12 ∞ 0.300 1.51633 64.14 13 ∞ 0.726 14 ∞ *ASPHERIC SURFACE

TABLE 20 EXAMPLE 10 • ASPHERIC SURFACE DATA SURFACE NUMBER KA A4 A6 A8 A10 2 3.6898607E−02 4.1325089E−02 7.7959667E−02 −3.1320039E−01 7.3615786E−01 3 −2.3337736E+01 −7.0438383E−02 1.2689897E−01 −1.6510709E−02 −3.3618937E−01 4 1.4512180E+00 1.0524624E−01 2.7959740E−01 −1.2882128E−01 −6.9518976E−01 5 3.1182039E+00 2.0460167E−01 9.3788710E−01 −3.1083520E+00 1.1989263E+01 6 7.0000900E−01 −1.7148265E−01 2.9051562E−01 −5.2650666E−02 1.2799215E+00 7 3.5470814E−01 −1.9176138E−01 1.7502659E−01 −3.4890662E−01 8.6734211E−01 8 −2.3602970E+00 −7.2840681E−02 −8.4242604E−01 2.9509268E+00 −8.6810396E+00 9 −1.8311731E+00 −2.6699460E−01 9.1126040E−02 −1.0539776E−01 1.2739701E−02 10  1.0044588E−01 −7.9144306E−01 7.1344844E−01 −2.9852745E−01 5.3475537E−02 11  −1.0909351E+01 −3.3970419E−01 2.9895759E−01 −1.5487925E−01 5.0278107E−02 A12 A14 A16 2 −1.2805754E+00 1.0422927E+00 −4.0402215E−01 3 −3.1710410E−01 1.2488311E+00 −7.8867528E−01 4 8.8551140E−01 3.3513814E−01 −5.9764108E−01 5 −2.7274104E+01 4.1138655E+01 −2.6221811E+01 6 −6.0805643E−01 −6.5701417E+00 1.0955959E+01 7 −1.2626762E+00 8.7271985E−01 −1.2234385E−01 8 1.3687948E+01 −1.1500705E+01 3.7304276E+00 9 −7.4356044E−02 6.4549028E−02 −1.2957543E−02 10  1.5902396E−03 −1.9540075E−03 1.7122320E−04 11  −9.7894164E−03 1.0056192E−03 −4.1181094E−05

TABLE 21 EXAMPLE 11 Si Ri Di Ndj νdj  1 ∞ 0.000 (APERTURE STOP) *2 1.50314 0.535 1.53049 56.50 *3 628.41695 0.115 *4 −4.44531 0.370 1.62272 23.21 *5 −62.81988 0.637 *6 −4.17719 0.469 1.58023 35.97 *7 −6.40179 0.594 *8 −104.73546 0.424 1.63400 23.43 *9 −6.00379 0.400 *10  −15.12220 0.684 1.53001 56.56 *11  2.46325 0.490 12 ∞ 0.210 1.51633 64.14 13 ∞ 0.394 14 ∞ *ASPHERIC SURFACE

TABLE 22 EXAMPLE 11 • ASPHERIC SURFACE DATA SURFACE NUMBER KA A3 A4 A5 A6 2 −2.0365693E+01 0.0000000E+00 4.6608762E−01 6.2264170E+00 −5.0423972E+01 3 9.4243460E+00 0.0000000E+00 −3.8974648E−01 4.4559307E+00 −2.4151496E+01 4 −1.6620841E+01 0.0000000E+00 −5.2931980E−02 6.2703036E−01 1.0545577E+01 5 9.2607139E−01 0.0000000E+00 7.2695152E−01 −6.9511296E+00 4.2467376E+01 6 −2.4760740E+01 0.0000000E+00 −1.3047327E−01 2.4330135E+00 −1.7226290E+01 7 −6.7752965E+00 0.0000000E+00 1.8648074E−01 −4.3671603E−01 −2.0354020E+00 8 6.5588238E−01 0.0000000E+00 1.7506684E+00 −8.8378884E+00 2.6904187E+01 9 −2.0717889E−01 0.0000000E+00 2.3613459E+00 −7.9481912E+00 1.3125291E+01 10  4.7225205E+00 0.0000000E+00 1.3643615E+00 −2.6424994E+00 −6.4556732E+00 11  −4.0651215E+00 0.0000000E+00 2.7621535E−01 −8.3109265E−01 −9.3114867E−01 A7 A8 A9 A10 A11 2 1.8137743E+02 −3.5004843E+02 2.8350045E+02 1.9307054E+02 −6.3169709E+02 3 7.2871768E+01 −1.1195508E+02 1.2462216E+01 2.7229728E+02 −4.8435836E+02 4 −1.1445553E+02 5.0392311E+02 −1.1949911E+03 1.4744707E+03 −4.0454823E+02 5 −1.6371076E+02 4.2768735E+02 −7.4859151E+02 7.7077980E+02 −1.6831315E+02 6 5.8614310E+01 −1.1773102E+02 1.3432269E+02 −3.9494616E+01 −1.2881457E+02 7 1.3278377E+01 −3.6511980E+01 5.2998878E+01 −3.0643480E+01 −2.1830861E+01 8 −5.2233138E+01 6.1068047E+01 −3.7054091E+01 1.5832337E+00 1.4039265E+01 9 −1.1158499E+01 2.0825154E+00 3.4605010E+00 −7.7481130E−03 −4.9719040E+00 10  3.0542833E+01 −5.1745586E+01 4.8761547E+01 −2.7217236E+01 8.2753322E+00 11  5.2125282E+00 −7.7790765E+00 5.9569451E+00 −2.2931301E+00 9.7168883E−02 A12 A13 A14 A15 2 4.6265769E+02 1.6287253E+01 −1.7236525E+02 6.1029992E+01 3 3.4877314E+02 −5.0089208E+01 −6.8013251E+01 2.7966323E+01 4 −1.4221313E+03 2.1038490E+03 −1.2376242E+03 2.8052258E+02 5 −7.0520258E+02 1.0071072E+03 −5.9028661E+02 1.3453911E+02 6 2.2213602E+02 −1.6988467E+02 6.6524528E+01 −1.0820674E+01 7 5.2017462E+01 −3.9148179E+01 1.4133341E+01 −2.0643976E+00 8 −9.3393438E+00 2.1834569E+00 5.7083905E−02 −7.3356919E−02 9 5.0185950E+00 −2.3388096E+00 5.5230980E−01 −5.3575879E−02 10  −6.5126134E−01 −4.0676099E−01 1.3421928E−01 −1.3122928E−02 11  3.1712682E−01 −1.4398589E−01 2.7639801E−02 −2.0727099E−03

TABLE 23 VALUES IN CONDITIONAL EXPRESSIONS EXPRESSION NUMBER EXAMPLE 1 EXAMPLE 2 EXAMPLE 3 EXAMPLE 4 EXAMPLE 5 EXAMPLE 6 f 4.252 4.230 4.137 4.309 5.383 4.439 Bf 1.002 0.997 1.298 1.299 0.889 1.073 FNo. 2.4 2.4 2.4 2.5 3.3 2.9 2ω 68.0 68.0 70.0 70.0 64.8 73.8 TL/f 1.012 1.017 0.993 0.982 0.994 1.109 f1 2.210 2.092 2.317 2.338 2.883 2.987 f2 −3.921 −4.297 −3.828 −4.191 −8.826 −7.414 f3 −623.420 −97.313 −1028.929 −1005.943 −9.747 −144.308 f4 7.214 16.428 1.781 1.511 10.339 39.158 f5 −3.597 −4.430 −1.479 −1.197 −3.944 −7.869 f/f45 1 −0.530 −0.730 −0.185 −0.400 −0.706 −0.424 D6/f 2 0.140 0.168 0.052 0.062 0.081 0.083 EXPRESSION NUMBER EXAMPLE 7 EXAMPLE 8 EXAMPLE 9 EXAMPLE 10 EXAMPLE 11 f 4.413 4.390 5.956 4.428 5.135 Bf 1.051 1.067 2.438 1.424 1.022 FNo. 2.9 2.9 3.9 2.6 3.1 2ω 77.4 78.8 51.8 59.6 67.4 TL/f 1.116 1.106 0.868 0.991 1.022 f1 3.035 3.003 2.071 2.171 2.839 f2 −8.193 −8.245 −3.166 −3.551 −7.701 f3 −64.642 −87.887 −6.952 −13.383 −22.456 f4 88.750 85.097 2.736 6.674 10.029 f5 −9.925 −8.731 −2.454 −5.318 −3.943 f/f45 1 −0.382 −0.441 −0.112 −0.106 −0.691 D6/f 2 0.087 0.080 0.042 0.080 0.091 

What is claimed is:
 1. An imaging lens substantially consisting of, in order from an object side, five lenses of: a first lens that has a positive refractive power and has a meniscus shape which is convex toward the object side; a second lens that has a negative refractive power; a third lens that has a negative refractive power; a fourth lens that has a positive refractive power; and a fifth lens that has a negative refractive power and has an aspheric shape of which an image side surface has an extreme point, wherein the following conditional expression (1) is satisfied: −1<f/f45<−0.105  (1), where f is a focal length of a whole system, and f45 is a composite focal length of the fourth and fifth lenses.
 2. The imaging lens, as defined in claim 1, wherein among absolute values of respective focal lengths of the first to fifth lenses, the absolute value of the focal length of the third lens is the maximum.
 3. The imaging lens, as defined in claim 1, wherein an intersection point between an object side surface of the fourth lens and a principal ray with a maximum angle of view is positioned on the object side of an intersection point between the object side surface of the fourth lens and an optical axis.
 4. The imaging lens, as defined in claim 1, wherein an intersection point between an object side surface of the third lens and a principal ray with a maximum angle of view is positioned on the object side of an intersection point between the object side surface of the third lens and an optical axis.
 5. The imaging lens, as defined in claim 1, wherein the following conditional expression is further satisfied: 0.02<D6/f<0.3  (2), where D6 is a thickness of the third lens on an optical axis.
 6. The imaging lens, as defined in claim 1, wherein the following conditional expression is further satisfied: −0.9<f/f45<−0.105  (1-1).
 7. The imaging lens, as defined in claim 6, wherein the following conditional expression is further satisfied: −0.8<f/f45<−0.1  (1-2).
 8. The imaging lens, as defined in claim 1, wherein the following conditional expression is further satisfied: 0.03<D6/f<0.2  (2-1), where D6 is a thickness of the third lens on an optical axis.
 9. The imaging lens, as defined in claim 8, wherein the following conditional expression is further satisfied: 0.04<D6/f<0.18  (2-2).
 10. The imaging lens, as defined in claim 1, wherein the second lens is concave toward the image side.
 11. An imaging apparatus comprising: the imaging lens, as defined in claim
 1. 